Zhe Wang†
b,
Wen-Cong Xu†c,
Dachuan Zhangb,
Man Gaod,
Tao Chend,
Youyi Sun*a,
Shuofeng Liang*b and
Si Wu
*b
aSchool of Materials Science and Engineering, North University of China, Taiyuan 030051, China. E-mail: syyi@pku.edu.cn
bHefei National Research Center for Physical Sciences at the Microscale, Anhui Key Laboratory of Optoelectronic Science and Technology, Department of Polymer Science and Engineering, University of Science and Technology of China, Hefei 230026, China. E-mail: siwu@ustc.edu.cn; liangsf@ustc.edu.cn
cShock and Vibration of Engineering Materials and Structures Key Laboratory of Sichuan Province, Mianyang, Sichuan 621999, China
dGuangxi Proberoo Advanced Materials Co., Ltd, 41 Jianye Road, Liangqing District, Nanning 530221, China
First published on 13th August 2025
Molecular weight serves as a critical parameter governing the adhesive properties of polymer adhesives. Nevertheless, its influence on the reversible adhesion of azopolymers exhibiting photoinduced reversible solid-to-liquid transitions remains poorly understood. Here, we systematically elucidate how molecular weight modulates the reversible adhesion behavior of azopolymers. Three azopolymers (P1, P2, and P3) were synthesized by ring-opening metathesis polymerization (ROMP), with molecular weights strategically designed below, near, and above the entanglement molecular weight (Me), respectively. UV irradiation induces trans-to-cis isomerization of azobenzene moieties, while visible light triggers cis-to-trans isomerization. The azopolymers exhibit photoswitchable glass transition temperatures (Tgs) and viscous flow temperatures (Tfs). Crucially, molecular weight dictates the mechanism of photocontrolled reversible adhesion. For P1 and P2, the trans azopolymers exhibit stronger adhesion than the cis form does. However, this trend is reversed for P3, where the cis P3 surpasses trans P3 in terms of adhesive performance. These findings establish molecular weight engineering as a critical strategy for developing high-performance stimuli-responsive reversible adhesives.
Azobenzene is known for its ability to undergo reversible cis–trans photoisomerization, a property that can be harnessed in various applications.29–34 Recent studies have demonstrated that certain azobenzene-containing polymers (azopolymers) and other photoresponsive polymers exhibit photoinduced reversible solid-to-liquid transitions, which are influenced by their photoswitchable glass transition temperature (Tg) values.35–42 Trans azopolymers retain a solid-state with Tg values above room temperature, whereas cis azopolymers transition to a liquid state with Tg values below room temperature. This unique behavior positions azopolymers as promising candidates for reversible adhesives,43–50 imprinting,51–56 healable materials,57–60 solar energy storage,61 and photomechanical applications.62–65 Previous studies have shown that some monodisperse azopolymers exhibit photocontrolled reversible adhesion due to adhesion differences between their cis and trans isomers. However, regulating the sign (positive/negative) of this adhesion contrast remains a challenge, which is essential for developing and applying photoresponsive reversible adhesives. While molecular weight is a well-established determinant of adhesion strength in polymeric adhesives,66,67 its regulatory effects on the reversibility and adhesion performance of azopolymers remain underexplored.
In this study, we synthesized a series of azopolymers with varying molecular weights through ring-opening metathesis polymerization (ROMP). Three distinct azopolymers P1, P2, and P3 were systematically investigated, with molecular weights strategically positioned below, near, and above the entanglement molecular weight (Me). All these azopolymers exhibit photoswitchable Tgs and viscous flow temperatures (Tfs). Molecular weight emerged as a key determinant of photoresponsive behavior, with P3 exhibiting significantly elevated Tf values relative to those of P1 and P2. Furthermore, the molecular weight governed the photocontrolled adhesion performance: P1 functioned as a UV-weakened adhesive, P3 displayed UV-enhanced adhesion, and P2 remained largely unaffected by UV irradiation. These molecular-weight-dependent photoresponsive phenomena are rationalized by variations in polymer chain entanglement dynamics. Our findings highlight the critical role of molecular weight control in the design of effective reversible adhesives.
Azopolymers (P1, P2, and P3) with varying molecular weights were subsequently synthesized via ROMP (Fig. 1a). To regulate molecular weight, we systematically explored different polymerization conditions (Table 1) and evaluated the impact of catalysts G1, G2, H2, and G3 on the ROMP process. The number-average molecular weight (Mn), weight-average molecular weight (Mw), PDI, and conversion rates, were determined by GPC (Table 1).
Entry | [MM]a![]() ![]() |
Catalyst | [MM] (mol L−1) | Mnc (kg mol−1) | Mwd (kg mol−1) | PDIe | Conversionf | Timeg (min) |
---|---|---|---|---|---|---|---|---|
a Initial molar concentration of MM.b Initial molar concentration of catalyst.c Mn.d Mw.e PDIs (PDI = Mw/Mn) determined by GPC equipped with a refractive index detector using polystyrene standards.f Conversion of MM determined using GPC by comparing the relative integrations of the azopolymer and MM peaks in the RI trace.g The reaction time from the addition of the catalyst to the addition of the terminator. | ||||||||
1 | 100![]() ![]() |
G1 | 0.1 | 78 | 128 | 1.64 | 73% | 15 |
2 | 100![]() ![]() |
G2 | 0.1 | 57 | 86 | 1.52 | 90% | 15 |
3 | 100![]() ![]() |
H2 | 0.1 | 255 | 706 | 2.76 | 71% | 15 |
4 | 100![]() ![]() |
G3 | 0.1 | 79 | 107 | 1.35 | 95% | 15 |
5 | 100![]() ![]() |
G3 | 0.2 | 75 | 94 | 1.26 | 90% | 15 |
6 | 100![]() ![]() |
G3 | 0.4 | 64 | 74 | 1.15 | 96% | 15 |
7 (P1) | 20![]() ![]() |
G3 | 0.4 | 16 | 18 | 1.11 | 95% | 5 |
8 (P2) | 100![]() ![]() |
G3 | 0.4 | 68 | 77 | 1.13 | 90% | 5 |
9 (P3) | 300![]() ![]() |
G3 | 0.4 | 233 | 276 | 1.19 | 94% | 5 |
10 | 500![]() ![]() |
G3 | 0.4 | 365 | 487 | 1.33 | 88% | 5 |
Among the tested catalysts, G3 achieved a higher conversion rate (95%), a narrow PDI (1.35), and an experimental Mn (75 kg mol−1) close to the theoretical Mn (61 kg mol−1) (Table 1, entry 4). In contrast, G1 and G2 exhibited broader PDIs, resulting in secondary metathesis reactions.68 While H2 caused rapid gelation and the formation of insoluble solids within seconds (Table 1, entry 3 and Fig. S5). Based on these findings, G3 was selected for further experiments.
Since ROMP is governed by Gibbs free energy, the monomer concentration ([MM]) plays a crucial role in polymerization kinetics. We systematically investigated the effect of [MM] on ROMP (Table 1, entries 4–6). At lower concentrations, GPC traces exhibited acromion peaks, indicating intermolecular and intramolecular chain transfer reactions.69 As [MM] increased to 0.4 mol L−1, these acromion peaks completely disappeared, yielding an azopolymer with a narrow PDI (1.15) (Fig. S6).
The reaction kinetics of azopolymer synthesis via ROMP were analyzed. Real-time monitoring revealed a progressive decrease in the monomer concentration during polymerization, accompanied by a distinct shift of the polymer peak in GPC curves toward shorter elution times (Fig. 1b and S7), indicative of increasing molecular weight. Within the initial period, ln([M0]/[M]) exhibited a linear relationship with time, confirming that ROMP follows first-order kinetics in this interval (Fig. S7). Between 3 and 5 minutes, molecular weight and PDI increased gradually. After 15 minutes, molecular weight plateaued, while PDI increased sharply, indicating the onset of chain transfer reactions. Based on these kinetics, 5 minutes was identified as the optimal reaction time, achieving a conversion rate of ∼90%, yielding an azopolymer with an Mn of 68 kg mol−1 and a PDI of 1.13.
Under these optimized conditions, we synthesized azopolymers with varying molecular weights by adjusting the monomer/catalyst feed ratio (Table 1, entries 7–10). As the feed ratio increased, Mn increased linearly (Fig. 1c and d), closely matching theoretical predictions, with high conversion rates and low PDI values, confirming that the polymerization proceeded in a controlled manner.
To elucidate the molecular weight dependence of azopolymer properties, three distinct azopolymers P1, P2, and P3 with controlled molecular weights of 16 kg mol−1, 68 kg mol−1, and 233 kg mol−1, respectively, were selected for comparative analysis (Table 1 and Fig. S8). Me of the trans azopolymer was ∼38 kg mol−1 (Fig. S10 and S11), estimated based on a reported method.70 Thus, P1, P2, and P3 represent polymers with Mn values below, slightly above, and substantially above Me, respectively.
The TGA curves revealed that all azopolymers decomposed at temperatures exceeding 300 °C, indicating high thermal stability of azopolymers (Fig. S12). SAXS, and WAXS data confirmed the formation of mesophases within the azopolymers (Fig. S13). Polarized optical microscopy (POM) images revealed small anisotropic grains dispersed within a largely isotropic matrix (Fig. S14), suggesting that the azopolymers exhibit characteristics of semicrystalline polymers, with both isotropic and anisotropic domains.
Tensile tests were performed to assess the effects of molecular weight on mechanical properties of azopolymers. P1 was brittle and could not form a free-standing specimen for test (Fig. 2a). In contrast, P2 formed stable, free-standing specimens, which exhibited an elongation at break of 11.69 ± 1.78% and a tensile strength of 15.11 ± 0.42 MPa (Fig. 2b). Notably, P3 demonstrated exceptional mechanical performance with a fracture elongation of 284.67 ± 5.39%, representing a 24-fold increase over P2, while retaining comparable tensile strength at 16.56 ± 0.44 MPa (Fig. 2c). This enhancement is attributed to Mn of P3 being significantly greater than that of Me, leading to increased entanglements and elasticity.
Moreover, P3 exhibited excellent reprocessability due to its linear polymer chain structure. A P3 specimen was hot-pressed and reprocessed three times and retained consistent mechanical performance after each cycle (Fig. 2d–f), demonstrating its potential for sustainable applications.
The above results establish molecular weight as a critical determinant of the mechanical performance of azopolymers. Next, we examined its governing effects on photoresponsive behavior. Fig. 3a compares UV-vis absorption spectra of P1 in THF solution and annealed film states. The π–π* transition band displays a blue shift and broadening in the annealed film compared to solution, which is attributed to the aggregation and out-of-plane orientation of azobenzene chromophore.71
Azobenzene aggregates are typically classified as H-aggregates or J-aggregates, depending on the angle between coplanar transition dipoles and the interconnecting axis (Fig. 3b). To quantify these aggregates, we employed a Gaussian curve-fitting procedure on the absorption spectra, decomposing the contributions from H-aggregates, J-aggregates, and free azobenzene groups (Fig. 3c–e). In the azopolymer films of P1, P2 and P3, the estimated relative proportions were ∼55% H-aggregates, ∼40% free azobenzene groups, and ∼5% J-aggregates. Notably, molecular weight had minimal influence on aggregate proportions, suggesting that aggregation is governed primarily by chromophore interactions rather than polymer chain length effects.
The azopolymer films exhibit reversible cis–trans photoisomerization upon alternating UV and visible light irradiation (Fig. 4a). In the as-prepared state, azobenzene chromophores predominantly adopt the thermodynamically stable trans configuration.
Upon UV irradiation, the π–π* absorption band at ∼350 nm decreases, while the n–π* absorption band at ∼440 nm increases, indicating a trans-to-cis isomerization (Fig. 4b–d). Subsequent visible light irradiation restored the original π–π* absorption band at ∼350 nm and reduces the n–π* absorption at ∼440 nm, indicating cis-to-trans isomerization (Fig. 4b–d). The π–π* absorption band of trans azobenzene is at ∼350 nm and that of cis azobenzene is at ∼310 nm, the blue shift of absorption band after UV irradiation and red shift after visible light irradiation indicate cis–trans isomerization of azobenzene. The maximum absorbance of azopolymer increased after a cyclic irradiation because the stacking states and orientation of the azobenzene changed.58,71 After UV and visible light irradiation, the estimated relative proportion of H-aggregates decreased, free azobenzene groups increased and J-aggregates remained roughly unchanged based on Gaussian curve-fitting procedure (Fig. 3, Fig. S15 and Table S1). Furthermore, the ratio of the absorbance of the π–π* band of trans-azobenzene groups (∼350 nm) to the φ–φ* band of phenyl groups (∼243 nm) serves as a useful parameter for determining azobenzene group orientation. Fig. 4b–d demonstrates that this ratio increases following UV and visible light irradiation, indicating that the azobenzene groups preferentially oriented perpendicular to the substrates prior to illumination.
These reversible spectral changes confirm that the azopolymers undergo repeatable cis–trans photoisomerization, demonstrating their potential for light-responsive applications (Fig. 4e–g).
Unlike previously reported azopolymers with similar structures,72 the azopolymers in this work exhibit photoinduced solid–liquid transition properties. We observed that trans-to-cis photoisomerization induced a solid-to-liquid transition of P1 (Fig. 5a). Upon UV irradiation (365 nm, 10.4 mW cm−2), the sharp edges of P1 powders gradually rounded, and some particles fused into droplets, indicating that photoinduced liquefaction occurred. In contrast, P2 and P3 powders exhibited negligible photoresponsive changes under UV irradiation (Fig. 5b and c). These results suggest that molecular weight plays a critical role in determining the photoinduced solid-to-liquid transition behavior of azopolymers.
![]() | ||
Fig. 5 Optical microscopy images of powders of (a) P1, (b) P2 and (c) P3 before and after UV irradiation (365 nm, 10.4 mW cm−2) for 5, 10 and 20 min at 25 °C. |
To elucidate the effect of molecular weight on the photoinduced solid-to-liquid transition of azopolymers, we conducted DSC and temperature-dependent rheology tests on trans and cis P1, P2 and P3. During the DSC heating process, all three azopolymers exhibited a similar phase transition temperature (∼61 °C), corresponding to their isotropic transitions (Fig. 6a–c). Notably, no distinct Tg was observed for the trans azopolymers.
We further examine the thermal behavior of the cis-azopolymers, (Fig. 6d–f). The cis-content, determined via 1H NMR integration, was 86%, 79%, and 90% for P1, P2 and P3, respectively (Fig. S9). In the first heating cycle, no clear Tg was detected, while an exothermic peak between 50 °C and 100 °C appeared, corresponding to the heat released during the cis-to-trans isomerization of azobenzene. During the subsequent heating cycle, the DSC curves of the cis azopolymers became identical to those of their trans counterparts, indicating complete thermal reversion of azobenzene to the trans form during the first heating cycle.
To further elucidate the effect of molecular weight on the thermal and viscoelastic properties of the azopolymers, we conducted temperature-dependent rheology tests on P1, P2, and P3 (Fig. 7).
In the temperature range of −10 °C to 60 °C, the storage moduli (G′) of the trans azopolymers remained around 2 × 108 Pa, while their loss moduli (G′′) were approximately 1 × 107 Pa, consistently lower than G′ (Fig. 7a–c). These results indicate that the azopolymers exhibited solid-like behavior within this temperature range. However, as the temperature increased to 60 °C, both G′ and G′′ dropped sharply. For P1 and P2, G′′ exceeded G′, marking the onset of viscous flow at 60 °C, in agreement with DSC data (Fig. 7a and b; Table 2).
Azopolymer | Tda (°C) | trans Tgb (°C) | trans Tfc (°C) | cis Tgb (°C) | cis Tfc (°C) |
---|---|---|---|---|---|
a Decomposition temperature (Td) measured at 95 wt% remaining during TGA under nitrogen (Fig. S12).b Tg values were determined using the decline in G′ by rheology.c Tf values were determined using the crossover of G′ and G′′ by rheology. The cis contents of azobenzene groups for P1, P2 and P3 were 86%, 79% and 90%, respectively (Fig. S9). | |||||
P1 | 342 | 57 | 60 | −4 | −3 |
P2 | 342 | 57 | 60 | −3 | 0 |
P3 | 342 | 59 | 114 | −1 | 93 |
In contrast, P3 exhibited a distinct rubbery plateau between 60 °C and 114 °C, with G′ remaining higher than G′′ (Fig. 7c). This behavior suggests significant chain entanglement, which delays the transition to the viscous flow regime. Upon further heating to 114 °C, G′′ eventually surpassed G′, defining the Tf of P3 (Table 2). Additionally, changes in the slope of G′ were observed for all samples, corresponding to Tg (Table 2). These findings demonstrate that increasing molecular weight enhances entanglement effects, leading to increased polymer melt viscosity.
Upon UV irradiation, trans azopolymers were converted to their cis counterparts (Fig. S9). The cis azopolymers exhibited a lower Tg, ranging from −4 °C to −1 °C, indicating that azopolymers possess photoswitchable Tgs (Fig. 7d–f; Table 2). Notably, molecular weight significantly influenced Tfs of cis azopolymers. Cis P1 displayed no rubbery plateau above Tg, and a Tf value of −3 °C (Fig. 7d); Cis P2 exhibited comparable G′ and G′′ in the range of ∼20 °C −50 °C, suggesting a Tf value of 0 °C (Fig. 7e); Cis P3 demonstrated a broad rubbery plateau between ∼25 °C −93 °C, and a Tf value of 93 °C (Fig. 7f). The underlying mechanism of difference of photoswitchable Tfs is attributed to the molecular weight dependence of chain entanglement. Rheological measurements identified a Me of 71 kg mol−1 for cis azopolymers (Fig. S10). Progressive molecular weight increases intensify chain entanglement effects, driving systematic elevation of Tf. Notably, cis P3 achieves markedly higher Tf values than P1 and P2 due to its Mn significantly exceeding the Me threshold.
Azopolymers have potential applications as photocontrolled adhesives. Azopolymer films were prepared by hot pressing at 100 °C, yielding uniform films with a thickness of 60 μm. The films were then cut into 5 mm × 5 mm pieces using a blade and sandwiched between two quartz slides, secured with clamps. The assembly was annealed at 80 °C for 2 hours, followed by cooling to room temperature to ensure strong adhesion, yielding the trans annealed samples, which were tested directly. For the cis samples, the trans samples were further irradiated at 365 nm (40.7 mW cm−2) for 10 minutes, followed by testing under light-protected conditions.
To investigate the effects of molecular weight on adhesion properties, we performed lap joint shear strength tests of trans P1, P2, and P3 at different temperatures (Fig. 8a). The adhesion strength of trans azopolymers increased with increasing molecular weight (Fig. 8b).
Specifically, for P1, P2, and P3, adhesion strength remained relatively stable between 25 °C and 50 °C but decreased significantly when the temperature increased to 70 °C (Fig. 8b–e). These results indicate that adhesion strength decreases sharply when the temperature exceeds the Tg of the azopolymer. However, this trend is partially mitigated by increasing molecular weight, as increased chain entanglement enhances adhesion retention at elevated temperatures.
Since molecular weight regulates the photoswitchable Tgs and Tfs of azopolymers, we hypothesized that it could also influence photocontrolled adhesion. At room temperature, the adhesion strengths of specimens bonded with trans P1, P2, and P3 were 1.19 ± 0.25, 2.06 ± 0.60, and 2.61 ± 0.25 MPa, respectively (Fig. 9a–c), indicating a positive correlation between adhesion strength and molecular weight. Upon UV irradiation, distinct adhesion responses were observed. The adhesion of the P1-bonded specimen decreased significantly to 0.20 ± 0.13 MPa, while that of P2 exhibited only a slight reduction (2.06 ± 0.60 to 1.73 ± 0.34 MPa). Notably, the P3-bonded specimen showed an increase in adhesion to 6.05 ± 1.23 MPa (Fig. 9f).
The observed changes in photocontrolled adhesion changes for P1, P2, and P3 arise from the interplay of two opposing factors: photoswitchable Tgs and Tfs reduce adhesion by softening the polymer matrix and trans-to-cis isomerization increases the dipole moment of azobenzene groups, enhancing polymer-substrate interactions.5,24 To quantify the effect of dipole moments, theoretical calculations using the Gaussian 16 package were performed. The cis azopolymer units exhibited a dipole moment of 4.45 Debye, significantly greater than the 2.49 Debye of the trans form (Fig. 9d, e, and Fig. S16). As molecular weight increases, both the Tfs and viscosity values of cis azopolymers gradually rise. Consequently, cis P1 with lower molecular weights flow more readily. For P1, the photoswitchable Tgs and Tfs dominated, leading to a substantial loss of adhesion upon UV irradiation. Dipolar interactions cannot sustain strong adhesion of highly fluid cis P1, leading to adhesion failure. In contrast, cis P3 retained a viscoelastic character at room temperature, with a modulus two orders of magnitude higher than that of cis P1, making the photoswitchable Tgs and Tfs less effective in reducing adhesion. Instead, the increased dipole moment became the dominant factor. Conversely, the high viscosity of cis P3 restricts flow, enabling it to maintain robust adhesion strength through dipolar interactions. For P2, these opposing effects nearly cancel each other, resulting in minimal adhesion changes upon UV exposure.
As a result, P1 and P3 function as UV-weakened and UV- enhanced adhesives, respectively. A quartz-slide assembly bonded with P1 was able to hold a 2 kg dumbbell, but upon UV irradiation, the dumbbell dropped due to adhesion loss (Fig. 9g). Conversely, P3-bonded slides supported twice the initial load after UV irradiation, demonstrating significantly enhanced adhesion (Fig. 9h). The photocontrolled adhesion was highly stable, with five UV irradiation-thermal annealing cycles showing negligible performance degradation (Fig. 9i–k). These results highlight the ability to precisely tune azopolymer adhesion by adjusting molecular weight, enabling the design of both photo-weakened adhesives and photo-enhanced adhesives for diverse applications.
Footnote |
† These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2025 |